8th Aerodynamic Decelerator and Balloon Technology Conference 1984
DOI: 10.2514/6.1984-794
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A method for calculating the pressure field about a ribbon parachutecanopy in steady descent

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Cited by 4 publications
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“…(2) in Eq. (5), one has (5) *'~~FS oq (6) ' Ik Equation (6) may be decomposed into two parts as where the terms containing the strength of the nascent vortices represent the velocity induced at the tip of the camber by the nascent vortices and (-u 0 + iv 0 ) 9 the velocity at the tip due to all other vortices (and their images), the doublet at the center of the circle in the f plane, and the ambient velocity. Equation (7) represents two coupled equations for the strengths and positions of the nascent vortices.…”
Section: (4) 47tmentioning
confidence: 97%
“…(2) in Eq. (5), one has (5) *'~~FS oq (6) ' Ik Equation (6) may be decomposed into two parts as where the terms containing the strength of the nascent vortices represent the velocity induced at the tip of the camber by the nascent vortices and (-u 0 + iv 0 ) 9 the velocity at the tip due to all other vortices (and their images), the doublet at the center of the circle in the f plane, and the ambient velocity. Equation (7) represents two coupled equations for the strengths and positions of the nascent vortices.…”
Section: (4) 47tmentioning
confidence: 97%
“…The vortex sheet analysis was used by Klimas [3] to derive the acceleration-independent apparent mass coefficient for arbitrarily shaped axisymmetric surfaces. Muramoto and Garard [4] used a continuous-source model to predict the steady-state drag of ribbon parachutes. None of the analyses dealt with the evolution of the unsteady wake and its interaction with the canopy.…”
Section: Introductionmentioning
confidence: 99%